potential function

Tags: #definition

potential function

Given an electrical network G=(V,E), a potential function U:V→R is an assignment such that for all u→ev, Ve=Uv−Ue, defined up to scaling by a constant.
The existence of such a function is equivalent to Kirchoff's second law

The nice thing about this formulation is that it's independent of direction.

Ohm's law then may be rewritten as

Ie=Uv−UuRe

and the first law is equivalent to for all vertices vi connected to v for v not connected to the battery

∑iUv−UviRi=0

We can combine all the Uv terms together to get

(1R1+⋯+1Rd)Uv−∑iUviRi=0

If v=1, then this would be equal to Ibat
If v=n, then this would be equal to −Ibat

Connection to Kirchoff's matrix

The first law is equivalent to saying that for U→ the vector of all potentials U→=[U1,…,Un]T

KU→=[Ibat0⋮0−Ibat]$$where$K$is[[Zettelkasten/Unfiled/Kirchoff′smatrixofanelectricalnetwork∥Kirchoff′smatrixofanelectricalnetwork]].However,$K$isdegenerateastherearemanysolutionsfor$U→$uptoscaling.Thus,we"ground"thenetworkbysetting$Un=0$.

\tilde{K} \begin{bmatrix}
U_1 \
\vdots \
U_{n-1}
\end{bmatrix} = \begin{bmatrix}
I_{bat} \
0 \
\vdots \
0
\end

where$K~$isthe[[Zettelkasten/Unfiled/reducedLaplacianmatrix∥reducedLaplacianmatrix]](asweremovedthe$n$throwandcolumn).Furthermore,wecanmaketheadditionalsimplifyingassumptionthat$Ibat=1$,thenrescaleafterwards.Then,notethatthe[[Zettelkasten/Unfiled/effectiveresistance∥effectiveresistance]]isthengivenby$U1$,ofwhichwemaysolvewith[[Zettelkasten/Unfiled/Cramer′srule∥Cramer′srule]].